http://www.cnr.it/ontology/cnr/individuo/prodotto/ID176520
Acoustic waves in hydrogels: A bi-phasic model for ultrasound (Articolo in rivista)
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- Label
- Acoustic waves in hydrogels: A bi-phasic model for ultrasound (Articolo in rivista) (literal)
- Anno
- 2009-01-01T00:00:00+01:00 (literal)
- Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#doi
- 10.1016/j.msec.2008.07.036 (literal)
- Alternative label
Piero Chiarelli ;Antonio Lanatà ; Marina Carbone (2009)
Acoustic waves in hydrogels: A bi-phasic model for ultrasound
in Materials science & engineering. C, Biomimetic materials, sensors and systems (Print)
(literal)
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- Piero Chiarelli ;Antonio Lanatà ; Marina Carbone (literal)
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- ISI Web of Science (WOS) (literal)
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- National Council of Research of Italy, Moruzzi, 1-56100 Pisa, Italy Interdepartmental Research Center \"E. Piaggio\", Faculty of Engineering, University of Pisa, via Diotisalvi, 2-56126 Pisa, Italy (literal)
- Titolo
- Acoustic waves in hydrogels: A bi-phasic model for ultrasound (literal)
- Abstract
- In the present paper a continuum poroelastic model for high frequency acoustic waves in hydrogels has been developed. The model has been used to obtain the acoustic longitudinal wave equation for ultrasound. In order to obtain a satisfactory model for hydrogels, a viscoelastic force describing the interaction between the polymer network of the matrix and the bounded water is introduced. The model is validated by means of ultrasound (US) wave speed and attenuation measurements in polyvinylalcohol (PVA) hydrogel samples as a function of their water volume fraction \"?\" and polymer matrix cross-linking. Themodel predicts that the law??(1+?) for ultrasound attenuation can be applied as a function of the frequency
?, where ? is the frequency exponent of the polymer-boundedwater viscosity. This outcome canwell explain the attenuation of the US frequency in natural gelswhere ? is typically about 0.25÷0.50while the value for purewater is 1. The theory and experiments show that US attenuation in hydrogels decreases steadily with the increase of its water volume fraction ? in a linear. The newproposed dissipativemechanismleads to a USwave speed c that follows the law: c=cw(?-?)-3/2, where cw is the US wave speed in water and ? is the volume fraction of the bounded water. Since 0b?b1 and ?N0, the hydrogel US velocity is always higher than that of pure water. If ? tends to 1 (100% water), then the US speed in hydrogels converges to a higher value than that of pure water. The US speed gap at ?=1, between hydrogels and water, is the direct consequence of the introduction of the polymer network-bounded water interaction. This is in linewith the experimental results that show that the US speed gap at?=1 decreases in the gel samples with amore cross-linked polymermatrix that has a lower bounded water volume fraction. On the contrary, if thewater content is very low(i.e., ?b0.4), the measured US speed converges to that of the dry hydrogelmatrixwhich increases in the samples with a higher degree of network cross-linkingwith greater elastic moduli. (literal)
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